[0007]According to the invention, the stated object is achieved, first of all, and essentially in the case of the mass flowmeter under discussion in that more than two measurement tubes are provided, and in particular an even number of measurement tubes are provided. According to the invention, it has been found that an increase in the flow cross section and thus a Coriolis meter configuration which is suitable for higher mass flows can be achieved not only by increasing the nominal widths of the measurement tubes of the single-tube or two-tube mass flowmeters but also by providing further measurement tubes. The further measurement tubes advantageously make it possible to keep the oscillation behavior of the individual measurement tubes constant, and the measurement tubes can still be excited by oscillation generators which were previously suitable only for relatively small mass flowmeters, that is to say which could cope with only a relatively low mass flow rate. This means that it is also possible to produce mass flowmeters which are physically small in comparison to known single-tube or two-tube mass flowmeters, since the increase in the total flow cross section of the measurement tubes need not be compensated for by lengthening the measurement tubes since it is not essential to change the cross sections of the individual measurement tubes which are used.
[0008]It is particularly advantageous for the measurement tubes to be arranged closely—seen at right angles to the flow direction—that is to say for the flow cross section which is covered by the measurement tubes to be provided in as small an area as possible. According to the invention, when using standard measurement tubes, that is to say measurement tubes with a circular cross section, mass flowmeters allow the best possible utilization of space, and in any case utilize space considerably better than those mass flowmeters which use only a single measurement tube or two measurement tubes.
[0009]In one particularly preferred refinement of the mass flowmeter according to the invention, the measurement tubes are associated with measurement tube groups, with the measurement tubes in one measurement tube group being mechanically coupled to one another. This mechanical coupling does not refer to the couplings between the measurement tubes on the inlet and outlet sides, which necessarily result in the measurement tubes diverging or being joined together in connecting pieces on the inlet and outlet sides, with the connecting pieces being used with flanges which can connect the measurement tubes overall to a pipeline system. In fact, this refers to mechanical couplings which are provided within the oscillation area of the measurement tubes. The mechanical couplings between the measurement tubes of a measurement tube group result in the measurement tubes also being functionally associated with one another, and in simplification of the oscillation behavior of the measurement tube arrangement.
[0011]In another preferred refinement of the invention, the measurement tubes in a measurement tube group are connected to one another essentially over their entire extent—seen in the flow direction—and in particular are soldered or welded to one another. This mechanical coupling means that the measurement tubes in a measurement tube group are linked to one another without any remaining degrees of freedom for individual movement. Nevertheless, an arrangement such as this can be used to provide a mass flowmeter form which operates on the Coriolis principle and is more compact overall than is possible with single-tube or two-tube mass flowmeters.
[0012]Further preferred refinements of the invention are distinguished in that the measurement tubes or measurement tube groups are associated with one another in pairs, and each pair is equipped with separate oscillation generators and / or with separate oscillation sensors. This makes it possible to excite and to evaluate two different pairs of measurement tubes or measurement tube groups independently of one another, in particular to excite them independently of one another in different eigen forms and to evaluate the oscillations of the eigen forms separately, without the excited oscillations being mutually superimposed.